\relax 
\@writefile{toc}{\contentsline {section}{\numberline {1}The $J/\psi $ Meson}{1}}
\@writefile{toc}{\contentsline {section}{\numberline {2}Production of the $J/\psi $}{1}}
\@writefile{toc}{\contentsline {section}{\numberline {3}Decay of the \ensuremath  {J/{{\setbox 0=\hbox {$\@mathbf {x\global \edef 4{0}}$}}\mathchar "0120}}}{1}}
\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces Production of \ensuremath  {J/{{\setbox 0=\hbox {$\@mathbf {x\global \edef 4{0}}$}}\mathchar "0120}}\ in \ensuremath  {e^+e^-}\ collisions.}}{3}}
\newlabel{fig:eejpsi}{{1}{3}}
\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces Production of \ensuremath  {J/{{\setbox 0=\hbox {$\@mathbf {x\global \edef 4{0}}$}}\mathchar "0120}}\ through gluon fusion. The open arrows show the direction of the color flow; recall arrows forward in time is color while those going backward in time are anti-color. }}{3}}
\newlabel{fig:ggfuse}{{2}{3}}
\@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces Direct decay of \ensuremath  {J/{{\setbox 0=\hbox {$\@mathbf {x\global \edef 4{0}}$}}\mathchar "0120}}\ into two $D$-mesons. This cannot occur for the \ensuremath  {J/{{\setbox 0=\hbox {$\@mathbf {x\global \edef 4{0}}$}}\mathchar "0120}}\ since the mass of the $D$-meson is more that half the mass of the \ensuremath  {J/{{\setbox 0=\hbox {$\@mathbf {x\global \edef 4{0}}$}}\mathchar "0120}}. }}{4}}
\newlabel{fig:psidd}{{3}{4}}
\@writefile{lof}{\contentsline {figure}{\numberline {4}{\ignorespaces The preferred method for the strong decay of the \ensuremath  {J/{{\setbox 0=\hbox {$\@mathbf {x\global \edef 4{0}}$}}\mathchar "0120}}. Note that three gluons are involved, this being the lowest number necessary to conserve all quantum numbers---one does not work since the initial state is colorless and the gluon has a net color. }}{4}}
\newlabel{fig:ozi}{{4}{4}}